Shift equation
Δλ = λC(1 − cos θ)
θ is the photon scattering angle from 0° to 180°.
Calculate wavelength shift, scattered wavelength, incident and scattered photon energy, and recoil electron kinetic energy from either incident wavelength or photon energy plus scattering angle.
Uses λC = h/(mec) = 2.42631023867 pm for an electron.
| Angle | 1 − cos θ | Δλ | λ′ | E′ | Energy loss |
|---|---|---|---|---|---|
| Run a calculation to compare common scattering angles. | |||||
Compton scattering describes how a photon loses energy when it scatters from a free electron. This calculator solves the common homework and lab quantities: wavelength shift, scattered wavelength, incident and scattered photon energy, and recoil electron kinetic energy.
Δλ = λC(1 − cos θ)
θ is the photon scattering angle from 0° to 180°.
λ′ = λ + Δλ
The outgoing photon wavelength is longer when θ > 0°.
E = hc/λ
Using hc = 1.239841984 keV·nm.
λC = h/(mec) = 2.42631023867 pm
Maximum electron shift = 2λC = 4.85262047734 pm.
Ke = Ein − Eout
This is the photon energy transferred to the electron in the simple model.
λ: incident wavelength; λ′: scattered wavelength; Δλ: shift; θ: scattering angle; me: electron rest mass.
The Compton wavelength h/(mec) ≈ 2.43 pm. Even big-angle scattering barely nudges visible light but meaningfully shifts X-rays.
Δλ peaks at 180°. Forward scatter (θ≈0°) barely changes energy.
E = hc/λ. A positive Δλ means lower photon energy and momentum—transferred to the electron.
Compton’s experiment showed light carries momentum like a particle, not just a wave—key evidence for photons.
At θ = 180°, the scattered photon has the lowest possible energy for a given input λ. This “backscatter edge” is used in detector calibration.
λC = 2.42631023867 pm and hc = 1.239841984 keV·nm.
Electron is initially at rest and effectively free; binding, Doppler broadening, and cross-section effects are not modeled.
Last reviewed: June 8, 2026.
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For an electron initially at rest, the maximum shift occurs at θ = 180° and equals 2λC, or 4.85262047734 pm.
The shift equation Δλ = λC(1 − cos θ) depends on angle and electron mass. The starting wavelength affects λ′ and the photon energies, but not the added wavelength shift.
Visible wavelengths are hundreds of nanometers, while λC is only about 0.002426 nm. Even the maximum shift is a tiny fraction of visible-light wavelength.
Calculate Δλ, add it to the incident wavelength to get λ′, then use E′ = hc/λ′. If you start from energy, convert to wavelength first with λ = hc/E.
It works best when the photon energy is large compared with electron binding energies and the electron can be treated as stationary before the collision.
The same form can be written with the target particle mass, but this calculator uses the electron mass. A proton or nucleus has a much smaller Compton wavelength, so the shift is much smaller.
The Compton wavelength λC is the constant h/(mec). The Compton shift Δλ is the actual angle-dependent increase λC(1 − cos θ).